A rigorous deduction of the thermodynamic-equilibrium condition is provided for a homogeneous, uncharged and linear dielectric fluid contained in an electrostatic field. Contrary to the previous ones, this deduction does not postulate the existence of a mechanical stress tensor and of a body force density in the polarized fluid. Then, the equilibrium condition is employed to obtain the mass density distribution of the fluid and to present a correct proof of the well-known formula for the attractive force between the plates of a plane-parallel capacitor immersed in the fluid. © 1994 Società Italiana di Fisica.

Barletta, A., Zanchini, E. (1994). Thermodynamic equilibrium in dielectric fluids. NUOVO CIMENTO DELLA SOCIETÀ ITALIANA DI FISICA. D CONDENSED MATTER, ATOMIC, MOLECULAR AND CHEMICAL PHYSICS, BIOPHYSICS, 16(2), 189-203 [10.1007/BF02451701].

Thermodynamic equilibrium in dielectric fluids

Barletta A.;Zanchini E.
1994

Abstract

A rigorous deduction of the thermodynamic-equilibrium condition is provided for a homogeneous, uncharged and linear dielectric fluid contained in an electrostatic field. Contrary to the previous ones, this deduction does not postulate the existence of a mechanical stress tensor and of a body force density in the polarized fluid. Then, the equilibrium condition is employed to obtain the mass density distribution of the fluid and to present a correct proof of the well-known formula for the attractive force between the plates of a plane-parallel capacitor immersed in the fluid. © 1994 Società Italiana di Fisica.
1994
Barletta, A., Zanchini, E. (1994). Thermodynamic equilibrium in dielectric fluids. NUOVO CIMENTO DELLA SOCIETÀ ITALIANA DI FISICA. D CONDENSED MATTER, ATOMIC, MOLECULAR AND CHEMICAL PHYSICS, BIOPHYSICS, 16(2), 189-203 [10.1007/BF02451701].
Barletta, A.; Zanchini, E.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/874340
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